Method for producing an opening in a metallic structural part

ABSTRACT

The invention relates to a method of producing an aperture ( 2 ) in a metallic component ( 1 ), in which the aperture ( 2 ) comprises, at least in certain portions, a non-cylindrically formed funnel ( 9 ), extends from a first surface ( 5 ) to a second surface ( 6 ) of a component wall ( 3 ) and is formed by a laser beam ( 10 ), it being attempted to improve the dimensional accuracy and reduce the roughness of the surface of the aperture and/or funnel in that, by appropriate choice of the laser parameters, the metal is predominantly removed by sublimation during the formation of the funnel ( 9 ) and the funnel ( 9 ) is formed by laser removal of layers ( 11 ) of a substantially constant thickness (FIG.  3 ).

[0001] The invention relates to a method of producing an aperture in a metallic component, in which the aperture comprises, at least in certain portions, a non-cylindrically formed funnel, extends from a first surface to a second surface of the component and is formed by a laser beam.

[0002] EP-A-0950463 discloses a method of forming a cooling hole comprising a diffuser portion, in which the diffuser portion is cut out by a beam-drilling method in such a way that the drilling beam remains within a previously selected cross-sectional area.

[0003] It is known from S. NOLTE, G. KAMLAGE: ‘Mikro-strukturierung mit Femtosekundenlasern’ [Micro-structuring with femtosecond lasers], LASEROPTO, Vol. 31, No. 3, Apr. 15, 1999 (1999-04-15), pages 72-76, XP000999012, that, during laser machining, an increasingly shorter pulse duration and a reduction in the ambient pressure assist the sublimation of the material and lead to an improved workpiece surface. In particular during laser-beam drilling, the striation of the hole and the drilling core can be improved by a reduction in the ambient pressure and by special process gases, such as helium.

[0004] U.S. Pat. No. 5,609,779 discloses a method of laser drilling non-circular apertures in a metallic component, in which the aperture comprises a diffuser which extends up to one surface of the component and is formed by vaporizing the metal by means of a laser, the laser beam traversing the surface from a centre line of the diffuser transversely to both sides at a respectively increasing rate and with overlapping laser spots, to allow non-circular apertures to be produced with a conventional laser as inexpensively as possible and with a relatively good surface. The increasing rate and the overlapping are intended to compensate for tolerances in the pulse energy which lead to varying material removal, and at the same time produce the specific, cross-sectionally non-circular form of the diffuser.

[0005] In this operation, it has proven to be problematical that the metal becomes liquid due to the pulse frequency and pulse duration used, which has adverse effects on the surface of the diffuser. Owing to the laser machining at an increasing rate, the thickness of the layers varies and decreases from the centre line outwards, whereby cumulative inaccuracies with regard to the form of the diffuser may occur, in particular in the case of a number of successive layers.

[0006] The object of the present invention is to provide a method of the generic type described at the beginning with which apertures can be formed with the best possible surface and dimensional accuracy.

[0007] The solution to the problem is characterized according to the invention in that, by choice of the laser parameters, such as for example the pulse frequency, pulse energy or pulse duration, the metallic material is predominantly removed by sublimation

[0008] by a generally more restricted movement of the laser or a superimposed movement.

[0009] Suitable laser parameters allow layers of substantially constant thickness of from 1 μm to 10 μm to be removed. The form and dimensions of the successively removed layers can be adapted to the form of the funnel, whereby the apertures can be produced economically without any finishing. The form of the funnel is substantially described by a first aperture angle, determining a height H of the funnel, and a second aperture angle, determining a width B. The funnel may alternatively also be conically formed with a circular cross section.

[0010] For removing the layers, a laser beam can be moved in a number of neighbouring, generally parallel, paths over the respective surface of the component, the removal beginning at an outer surface of the metallic component and taking place, for example, line by line for each layer. An overlapping of the individual paths is not required and is avoided to carry out the method as efficiently as possible.

[0011] To realize layers of substantially constant thickness, the laser beam can move along the individual paths at a constant rate.

[0012] The laser removal can be carried out at a pulse frequency of from 1 to 50 kHz, in order to remove the material predominantly by sublimation during the forming of the aperture and/or the funnel. For this purpose, as much energy per pulse as possible must be introduced into the region to be removed over an extremely short period of time. To realize the extremely short period of time, the laser removal can be carried out with a pulse duration of from 10 to 1000 ns and a pulse energy of 0.005 to 1 Joule per pulse, these laser parameters allowing pulse peak outputs in the range from 50 kW to 1 MW to be achieved.

[0013] Before or after the forming of the funnel, a cross-sectionally substantially circular or cylindrical (aperture) portion of the aperture can be formed by laser drilling, so that the aperture comprises a non-cylindrically formed funnel and a substantially cylindrically formed (aperture) portion. During the laser drilling of the cylindrical (aperture) portion, the laser beam is aligned in the direction of the centre axis of the aperture, generally running at an acute angle in relation to the surface of the component.

[0014] During the removal of the layer, the laser beam can move spirally over the respective surface of the component, it being possible for the relative movement to begin at the centre, where the centre axis of the aperture intersects the outer surface of the component, or at the outer circumference of the funnel.

[0015] Further exemplary embodiments of the invention are described in the subclaims.

[0016] The invention is explained in more detail below on the basis of exemplary embodiments with reference to a drawing, in which:

[0017]FIG. 1 shows in a perspective representation a turbine blade of a gas turbine with apertures formed as cooling-air holes, which are produced according to a refinement of the method according to the invention,

[0018]FIG. 2 shows a cross-sectional view through a component wall in which a cylindrical aperture portion produced in a first step according to a refinement of the method according to the invention is represented,

[0019]FIG. 3 shows a cross-sectional view through a component wall in which an aperture produced according to a refinement of the method according to the invention is represented and

[0020]FIG. 4 shows a cross-sectional view through a component wall in which another aperture produced according to an alternative refinement of the method according to the invention is represented.

[0021]FIG. 1 shows as a metallic component a turbine blade 1 of a gas turbine, such as for example an aircraft engine, in a perspective representation, in which numerous apertures 2, formed as cooling-air holes, are formed by the method according to the invention. The cooling-air holes 2 generally run at an acute angle 4, shown in FIG. 2, through the component wall 3, which angle usually lies in the range from 12° to 35° in relation to an outer surface 6 of the component 1 and is, for example, 30°. From a cavity in the turbine blade 1, compressor air is passed through the cooling-air holes 2, in order to direct a film of cooling air over the outer surface 5 of the turbine blade 1.

[0022] The turbine blade 1 consists of a metal, such as for example an Ni- or Co-based alloy, and, for producing the apertures 2, is clamped in a suitable machine tool, in which it can be moved or turned along a number of axes. The relative movement between a laser with which the forming of the aperture 2 is performed by laser removal and the component 1 to be machined is generally produced by moving the component 1. Similarly, this can be achieved by a generally more restricted movement of the laser or a superimposed movement. FIG. 2 shows a sectioned view of the component wall 3 of the turbine blade 1, in which an aperture portion 7 produced in a first step according to an exemplary embodiment of the method according to the invention, having a substantially circular cross section, is represented. The centre axis 8 of this cylindrical aperture portion 7 runs at an acute angle 4 of approximately 30° through the component wall 3. As a consequence of this, in the plan view indicated merely by dashed lines, the circular cross section is represented in an elongated form in the inner, first surface 5 and the outer, second surface 6.

[0023] The apertures 2 produced by the method according to the invention are through-apertures and extend from the inner, first surface 5 to the outer, second surface 6 of the component wall 3. Before the forming of a cross-sectionally non-circular funnel 9, shown in FIG. 3, firstly, in a first step, the aperture portion 7 of circular cross section is formed by means of laser drilling. For this purpose, a schematically indicated laser beam 10 of an Nd-YAG laser is used and directed onto the outer, second surface 6 of the component wall 3 in the direction of the centre axis 8 of the aperture portion 7 to be drilled. The laser parameters, such as the pulse duration and pulse energy, as well as the number of pulses, are chosen according to the thickness of the component wall 3.

[0024] In the case of an exemplary embodiment of the method according to the invention, then, in a second step, the non-cylindrical funnel 9, represented in FIG. 3, is formed, respectively comprised by the cooling-air holes 2 for reasons of flow dynamics, in order to increase the pressure of the air flowing through. For this purpose, by suitable choice of the laser parameters, the metallic material is sublimated during the laser removal, beginning from the outer, second surface 6, so that the metal substantially does not go into the liquid phase and no viscous material can be deposited in the region to be removed, thereby impairing the quality of the surface.

[0025] The forming of the funnel 9 takes place by substantially parallel layers 11, which in FIG. 3 are indicated schematically by dashed lines and greatly enlarged, being removed with respect to the outer, second surface 6. The laser removal takes place with a multiplicity of pulses of the laser beam 10, the pulse energy being adapted to the thickness of the layers 11 to be removed. Depending on the desired form of the funnel 9, the second aperture angle 14 of which, determining a width B, can vary in relation to the centre axis 8 and is, for example, approximately 15°, the thickness of the layers 11 lies between 1 μm and 10 μm. The material of the individual layers 11 is respectively removed by laser in paths 12 indicated by dashed lines and greatly enlarged, in which the laser beam 10 moves line by line in relation to the surface 6 of the component 1. The movement along the paths 12 takes place at a constant rate. The paths 12 respectively extend over the entire width B or, in the case of another alignment, the entire height H of the funnel 9.

[0026] To ensure the sublimation of the metallic material of the component 1, a high pulse energy must be introduced by the laser beam 10 into the region to be removed with an extremely short pulse duration. For this purpose, the Nd-YAG laser is equipped with a Q-switch, and a pulse energy of from 5 to 100 mJoules per pulse, with a pulse duration of from 10 to 1000 ns, is chosen. Alternatively, along with the Nd-YAG drilling laser, a separate Q-switch Nd-YAG laser can be used.

[0027] In the plan view indicated by dashed lines in FIG. 3 of the outer, second surface 6 of the component wall 3, it can be seen that the dimensions of the funnel 9 are chosen such that a height H resulting from a first aperture angle 13 is smaller than the width B of the funnel 9. In the case of the present exemplary embodiment, the height H corresponds to the diameter D of the aperture portion 7. The funnel 9 has the same centre axis 8 as the aperture portion 7 and consequently runs coaxially in relation to the latter. The funnel 9 and the cylindrical aperture portion 7 together form the aperture 2.

[0028]FIG. 4 shows in a cross-sectional view another aperture 2, formed as a cooling-air hole, which is produced by an alternative refinement of the method according to the invention. It is also the case with this cooling-air hole 2 that, firstly, an aperture portion 7 of substantially circular cross section is formed by laser drilling at an acute angle 4 of approximately 30° in relation to the outer, second surface 6 of the component wall 3 of the turbine blade 1. The laser beam 10 of the Nd-YAG laser is in this case aligned in the direction of the centre axis 8 of the aperture portion 7.

[0029] In a second step, the funnel 9 is then formed by laser removal, beginning from the outer, second surface 6 of the component wall 3. In this case, the Nd-YAG laser is equipped with a Q-switch and, by appropriate choice of the laser parameters, is capable of sublimating virtually completely the metallic material to be removed for the forming of the funnel 9. Alternatively, for the second step, a separate Q-switch Nd-YAG laser can be used along with the Nd-YAG drilling laser used in the first step. In order to introduce into the material to be removed the pulse peak output required for this purpose, in the range from 50 kW to 1 MW, a pulse energy of from 0.005 to 0.1 Joule per pulse and a pulse duration of 10 to 1000 ns are provided.

[0030] The thickness of the respective layer 11 is chosen according to the form of the funnel 9. This thickness generally lies in the range from 1 μm to 10 μm. In the plan view indicated by dashed lines in FIG. 4, it can be seen that a width B of the funnel 9 extends substantially symmetrically in relation to the centre axis 8 of the aperture 2. The height H of the funnel 9 extends asymmetrically in relation to the centre axis 8, since, as can be seen well in the cross-sectional view of FIG. 4, the first aperture angle 13 in relation to the centre axis 8 towards one side is large and is approximately 16°. As a result, the funnel 9 deviates away from the centre axis 8 of the aperture 2 more strongly on one side.

[0031] The layers 11 are respectively removed in the paths 12 indicated by dashed lines, in which the laser beam 10 moves at a constant rate in relation to the component 1. The thickness of the layers 11 is adapted in each exemplary embodiment of the method according to the invention to the form of the funnel 9, which is substantially described by the first aperture angle 13, determining the height H, and the second aperture angle 14, determining the width B. The funnel 9 may also be formed conically with a circular cross section.

[0032] In all the refinements of the method according to the invention, the funnel 9 may be initially produced at the outer, second surface 6 of the component wall 3 by laser removal by means of an Nd-YAG laser equipped with a Q-switch and, following that, in a second step, the aperture portion 7 of substantially circular cross section may be produced by laser drilling with an Nd-YAG laser, the funnel 9 and the cylindrical aperture portion 7 here again having a common centre axis 8. The form of the funnel 9 may be symmetrical or asymmetrical in relation to the centre axis 8, depending on the requirement, as a result of the choice of the aperture angle 13 and its dimensions H and B.

[0033] In a further refinement of the method according to the invention, the material of the individual layers 11 may be removed by the laser beam 10 moving spirally around the centre axis 8 of the aperture 2 in relation to the outer surface 6 of the metallic component 1. 

1. Method of producing an aperture in a metallic component, in which the aperture (2) comprises, at least in certain portions, a non-cylindrically formed funnel (9), extends from a first surface (5) to a second surface (6) of a component wall (3) and is formed by a laser beam (10), characterized in that, by choice of the laser parameters, the metal is predominantly removed by sublimation during the formation of the funnel (9) and the funnel (9) is formed by laser removal of layers (11) of a substantially constant thickness, in which method, during the removal of the layers (11), the laser beam (10) moves in a number of neighbouring paths (12), adapted in length and number to the form of the funnel (9), over the respective surface (6) of the component (1).
 2. Method according to claim 1, characterized in that, during the removal of the layers (11), the laser beam (10) moves at a constant rate in relation to the respective surface (5, 6) of the component wall (3).
 3. Method according to claim 1 or 2, characterized in that the layers (11) are removed with a substantially constant thickness of from 1 μm to 10 μm.
 4. Method according to one or more of the preceding claims, characterized in that the form and dimensions of the layers (11) are adapted to the form of the funnel (9).
 5. Method according to one or more of the preceding claims, characterized in that the laser beam (10) moves along the individual paths (12) at a constant rate.
 6. Method according to one or more of the preceding claims, characterized in that the laser removal is carried out at a pulse frequency of from 1 to 50 kHz.
 7. Method according to one or more of the preceding claims, characterized in that the laser removal is carried out with a pulse duration of from 10 ns to 1000 ns.
 8. Method according to one or more of the preceding claims, characterized in that the laser removal is carried out with pulse peak outputs in the range from 50 kW to 1 MW.
 9. Method according to one or more of the preceding claims, characterized in that, before or after the forming of the funnel (9), a cross-sectionally circular portion (7) of the aperture (2) is formed by laser drilling.
 10. Method according to one or more of the preceding claims, characterized in that, during removal of the layers (11), the laser beam (10) is moved in a spiral path. 